Charmed baryon Λc in nuclear matter

Abstract

Density dependences of the mass and self-energies of ${\mathrm{\ensuremath{\Lambda}}}_{c}$ in nuclear matter are studied in the parity projected QCD sum rule. Effects of nuclear matter are taken into account through the quark and gluon condensates. It is found that the four-quark condensates give dominant contributions. As the density dependences of the four-quark condensates are not known well, we examine two hypotheses. One is based on the factorization hypothesis (F-type) and the other is derived from the perturbative chiral quark model (QM-type). The F-type strongly depends on density, while the QM-type gives a weaker dependence. It is found that, for the F-type dependence, the energy of ${\mathrm{\ensuremath{\Lambda}}}_{c}$ increases as the density of nuclear matter grows, that is, ${\mathrm{\ensuremath{\Lambda}}}_{c}$ feels repulsion. On the other hand, the QM-type predicts a weak attraction ($\ensuremath{\sim}20$ MeV at the normal nuclear density) for ${\mathrm{\ensuremath{\Lambda}}}_{c}$ in nuclear matter. We carry out a similar analysis of the $\mathrm{\ensuremath{\Lambda}}$ hyperon and find that the F-type density dependence is too strong to explain the observed binding energy of $\mathrm{\ensuremath{\Lambda}}$ in nuclei. Thus we conclude that the weak density dependence of the four-quark condensate is more realistic. The scalar and vector self-energies of ${\mathrm{\ensuremath{\Lambda}}}_{c}$ for the QM-type dependence are found to be much smaller than those of the light baryons.